WO2004061490A1 - Filtre optique - Google Patents

Filtre optique Download PDF

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Publication number
WO2004061490A1
WO2004061490A1 PCT/EP2003/051068 EP0351068W WO2004061490A1 WO 2004061490 A1 WO2004061490 A1 WO 2004061490A1 EP 0351068 W EP0351068 W EP 0351068W WO 2004061490 A1 WO2004061490 A1 WO 2004061490A1
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WO
WIPO (PCT)
Prior art keywords
layer
layers
optical
optical filter
index
Prior art date
Application number
PCT/EP2003/051068
Other languages
English (en)
Inventor
Denny Wernham
John Russell
Glenn Morgan Jones
Original Assignee
Thales Uk Plc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Thales Uk Plc filed Critical Thales Uk Plc
Priority to DE60312557T priority Critical patent/DE60312557T2/de
Priority to JP2004564247A priority patent/JP2006511838A/ja
Priority to US10/539,623 priority patent/US8018652B2/en
Priority to EP03809192A priority patent/EP1573371B1/fr
Publication of WO2004061490A1 publication Critical patent/WO2004061490A1/fr

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Classifications

    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/02—Details
    • H01L31/0216—Coatings
    • H01L31/02161—Coatings for devices characterised by at least one potential jump barrier or surface barrier
    • H01L31/02167—Coatings for devices characterised by at least one potential jump barrier or surface barrier for solar cells
    • H01L31/02168—Coatings for devices characterised by at least one potential jump barrier or surface barrier for solar cells the coatings being antireflective or having enhancing optical properties for the solar cells
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00—Optical elements other than lenses
    • G02B5/20—Filters
    • G02B5/28—Interference filters
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00—Optical elements other than lenses
    • G02B5/20—Filters
    • G02B5/28—Interference filters
    • G02B5/281—Interference filters designed for the infrared light
    • G02B5/282—Interference filters designed for the infrared light reflecting for infrared and transparent for visible light, e.g. heat reflectors, laser protection
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00—Energy generation through renewable energy sources
    • Y02E10/50—Photovoltaic [PV] energy

Definitions

  • the present invention relates to optical filters in the form of oplical coatings applied to substrates.
  • the present invention relates particularly, though not exclusively, to optical filters for photovoltaic cells, especially solar cells.
  • Photovoltaic cells such as solar cells, typically possess a preferential optical operating spectrum across/within which it is desired to have the photovoltaic cell operate. This may be because the design of the cell causes it to be relatively efficient in respect of, or to be relatively sensitive to, optical radiation within such a preferential spectrum. Alternatively, or additionally, it may be the case that optical radiation outside the operating spectrum is in some way detrimental to the operation of the cell.
  • the efficiency of the photo-electrical conversion process of many photovoltaic cells falls as the temperature of the cell rises. Consequently, many solar cells employ filters designed to exclude from radiation incident upon the cell those wavelengths of radiation which have a propensity to heat the cell. Typically, the filters are designed to reflect incident
  • Infra-Red (IR) radiation Infra-Red (IR) radiation.
  • a single "band-pass" filter may be employed which is designed to simultaneously exclude not only IR radiation but also UV radiation from radiation incident upon a solar cell, but let “pass” through the filter optical radiation lying within a spectral band bounded by the excluded IR and UV radiations.
  • a silicon solar cell is operative responsive to radiation of wavelengths between 0.40 ⁇ m to 1.1 O ⁇ m. Solar energy outside of this band is generally not converted into electricity and when absorbed only heats up the solar cell thereby reducing its efficiency.
  • Certain types of optical band-pass filter comprise a mi.L i -layer stack structure arranged upon a substrate, such as a glass substrate.
  • Such multi-layer band-pass filters are designed to reflect IR radiation (or near-IR radiation) that lies immediately adjacent one side of a spectral band of radiation in respect of which a solar cell is intended to operate (e.g. O.'l ⁇ m to 1. ] ⁇ m wave engths) , to transmit optical radiation lying within that spectral band and to reflect UV lying adjacent the other side of the spectral band of the solar cell.
  • the band-pass transmission spectra of such multi-layer filters is achieved by forming the stack of layers from repeating pairs of adjacent layers in which any one layer of a pair is comprised of material having an index of refraction which differs from the index of refraction of the other layer of the pair.
  • the resulting multilayer stack has an index of refraction which periodically jumps between two values as the depth of the multi-layer stack increases.
  • the "optical thickness" of a layer is given by multiplying the physical thickness of the layer by the index of refraction of the material of the layer for a particular wavelength of optical radiation.
  • a layer of constant physical thickness will have an optical thickness which depends upon the wavelength of optical radiation passing through it.
  • the multi-layer stack By appropriately controlling the physical thickness of each of the two layers in the repeated pair of layers such that each has an optical thickness equal to of a predetermined optical "design" wavelength (e.g. an IR wavelength) , the multi-layer stack causes reflection of optical radiation to occur not only at (and around) the predetermined "design” wavelength, but also at (and around) other wavelengths corresponding to "higher order" frequencies equal to an odd-integer multiple of the predetermined optical "design" wavelength (e.g. an IR wavelength)
  • a predetermined optical "design” wavelength e.g. an IR wavelength
  • such a quarter-wave stack may be employed as an optical filter for reflecting IR radiation by selecting the predetermined wavelength to be a suitable IR wavelength such that a reflection band is formed adjacent a desired spectral pass-band.
  • a drawback of such interference filters is that the aforementioned "higher order" reflection bands often reside well within the desired spectral pass-band. Thus, such filters may well reflect radiation which it is not desirable to reflect .
  • multi-stack optical interference filter has been proposed in which the multi-layer stack is composed of materials having three different refractive indices rather than just two.
  • the resultant structure is able to suppress the first few of the offending "higher order" reflection bands which usually occur m simple H - wave stacks as discussed above.
  • the strength of the multi-layer stack is sensitively dependent on the degree of interfacial adhesion between adjacent stack layers. Since adjacent layers in the aforementioned prior art devices are comprised of different materials, it is often the case that the differences (either chemical and/or physical) between such neighbouring layers reduce the strength of the interfacial bond which results in the interface being a primary site of structural weakness in the mult -layer stack.
  • the transmission spectrum thereof at regions in between successive reflection bands are not uniformly transmissive. That is to say, although the reflection bands of such interference filters are generally mainly confined to a limited spectral band, they are in fact not fully so confined. Rather, the so-called reflection "bands" often possess significant ripples or transients of non-zero optical reflectance in the filter at spectral regions within the pass-band thereof.
  • This spreading/dispersion of the reflection band into the pass-band is principally due to the discontinuity in refractive index occurring at the interface of successive layers of a stack. It is detrimental to the transmission spectrum of such filters since it attenuates optical radiation which it is intended to pass to an underlying solar cell. Hence, solar cell efficiency is reduced.
  • the present invention may provide an optical filter including a substrate having a plurality of layers of materials stacked upon it each of which layers is formed from one or both of: a first material having a first index of refraction; and, a second material having a second index of refraction being less than the first index of refraction; wherein the plurality of layers of materials include a first layer and a second layer each formed from an i homogeneous mixture of said first material and said second material and a third layer formed from the first material being stacked in between the first layer and the second layer wherein the optical thickness of each of said first and said second layers is greater than the optical thickness of said third layer.
  • the index of refraction of those layers varies with the depth of the layer between values greater than the second index of refraction and less than the first index of refraction.
  • an interference filter in the form of a multi-layer stack (on a substrate) comprising a repeating group of layers, the group including at least a relatively high refractive index layer sandwiched between two layers of varying (but lower) refractive index, one may for example, provide an interference filter which substantially reduces or suppresses ripples, oscillations or transients of non-zero optical reflectance that would otherwise tend to occur outside the main reflectance band, and "higher order" reflectance bands, of the multi-layer stack. That is to say, the transmission spectrum of the resulting multi-stack filter will tend to vary substantially more monotonicaliy within/across the pass-band of the filter, or if not monotonicaliy then will at least oscillate with lesser amplitudes therein.
  • the present invention is able to reduce or substantially remove any discontinuity in refractive index and material composition/structure as between adjacent layers of a multi-layer stack. Consequently, since a portion of an inhomogeneous layer immediately adjacent a neighbouring layer is materially very similar (or identical) to that neighbouring layer, the bonding of the two layers in question at their interface is enhanced thereby strengthening the multi-layer structure at that interface.
  • each of the "layers" of the optical filter of the present invention are formed from a particular choice of the proportions of the same two ingredient materials.
  • the term "layer” used herein therefore refers to strata of differing material composition occurring in a continuously formed object whereby each strata corresponds to a particular composition (s) in the material forming the. continuous object rather than corresponding merely to the collocation or joining of independent layers.
  • the "optical thickness" of a layer of material is given by multiplying the physical thickness of the layer by the index of refraction of that layer.
  • the optical thickness is given by integrating the depth-dependent refractive index across the depth of the layer in question.
  • the optical thickness of the first layer and of the second layer each differ in magnitude from a value 2Q by less than Q/2, and the optical thickness of the third layer differs in magnitude from the value Q by less than Q/2, where Q is the optical thickness of a given said layer traversed by substantially ⁇ of a wavelength of optical radiation of a common reference wavelength at which said optical thicknesses are determined.
  • the optical thickness of the first layer may be substantially equal to the optical thickness of the second layer, or the two said layers may differ in optical thickness.
  • the optical thickness of the first and second layers may or may not be equal in value to 2Q depending upon whether or not design optimisation requires this.
  • the optical thickness of the first Jayer and of the second layer may each be substant ally equal to the value 2Q.
  • the optical thickness of the third layer may also be varied when optimising design performance and may be substantially equal to the value Q or may differ from that value by an amount less than Q/2.
  • the optical filter includes, within its plurality of layers, a pair of outer layers each being formed from the first material and between which are stacked the first, second and third layers. This results in a five-layer nest including the first, second and third layers sandwiched between the pair of outer layers.
  • the optical thickness of each of the outer layers preferably differs in value from the magnitude Q by less than Q/2.
  • the optical thickness of the outer layers themselves may also individually bo varied within the aforementioned limits in order to assist in optimising the performance of the filter as a whole.
  • the optical thickness of each one of the pair of outer layers may differ from each other or may substantially equal to each. Where the optical thickness of each of the outer layers is substantially equal, this common optical thickness may be equal to Q or may differ from Q (by less than Q/2) .
  • Tt is to be understood that the term "inhomogeneous mixture" in respect of the mixing of materials of differing refractive index, is intended to refer to the nature of the relative proportions of mixed components (which form the mixture) being not homogeneous throughout at least part of the depth of the layer formed by the inhomogeneous mixture.
  • the result of the inhomogeneity of the mixture is a variation of the refractive index of the layer so formed between different depth locations in the same layer.
  • the index of refraction of the first and/or second layer may vary continuously through at least a part of the depth of the respective layer.
  • the index of refraction of the first and/or one second layer may vary substantially in a step-wise manner through at least a part of the depth of the respective layer.
  • the first and/or second layer may be a physically continuous article, not being physically discontinuous but having a spatial distribution (inhomogeneous) of mixture which causes sharp/rapid or substantially step-wise changes in the refractive index of the layer at certain regions of depth thereof where the mixture changes correspondingly sharply/rapidly or substantially in a step-wise way (or nearly so) .
  • the first and/or second layer may preferably comprise a plurality of sub-regions each of which is formed from a homogeneous mixture of the first material and the second material whereby the homogeneous mixture forming any one sub-region differs from the homogeneous mixture forming immediately neighbouring sub-regions within the intermediate layer such that the index of refraction of each of the plurality of sub-regions is substantially constant through the depth of the sub-region and the index of refraction of the respective first and/or second layer varies sharply/rapidly or substantially step-wise between successive sub-regions thereof.
  • neighbouring sub-regions of the digitised first/second layer may be physically continuously formed within one physically continuous respective layer.
  • one may cause the mixture to change substantially step-wise between neighbouring sub-regions thereby causing a corresponding "step” in the refractive index therebetween.
  • all variations in the index of refraction of the first and/or second layer may increase that index of refraction as the depth of the respective layer increases from regions thereof remote from the third layer to regions thereof proximate the third layer.
  • a refractive index "ramp” may have a smoothly varying refractive index ramp.
  • the plurality of layers are preferably arranged to form a stack of layers in which successive layers are arranged in a periodically repeating order across the depth of the stack.
  • the filter may be arranged to substantially reflect at least Infra-Red radiation and to transmit optical radiation at least in the visible optical spectrum.
  • the filter may be arranged to substantially reflect at least Infra-Red radiation and Ultra-violet radiation.
  • the present invention may also provide a cover for a photovoltaic cell comprising a filter according to the first aspect of the invention, and may comprise a photovoltaic cell comprising such a cover.
  • the photovoltaic cell is a preferably solar cell.
  • the present invention may provide an optical filter including a substrate having a layer arranged upon it formed from an inhomogeneous mixture of: a first material having a first index of refraction; and, a second material having a second index of refraction being less than the first index of refraction; the inhomogeneous mixture being such that the value of the index of refraction of the layer oscillates with the depth of the layer between values greater than the second index of refraction and less than the first index of refraction.
  • This may either be an alternative to, or may form a part of, a multi-layer stack type filter.
  • the oscillating variations in refractive index result in a filter having one main reflection band (which may be centred on an JR frequency) and has substantially no "higher order" type reflection bands. Since "higher order" reflection bands are suppressed in such a case, the filter is able to operate as an IR filter only with little or substantially no reflection of other wavelengths outside the single reflection band.
  • the oscillating variations of the value of the index of refraction of the layer may include at least some sharp/rapid or substantially step-wise variations, or the variations may be mostly (or only) such sharp/rapid or substantially step-wise variations.
  • the layer may preferably comprise a plurality of sub-regions each of which is formed from a homogeneous mixture of the first material and the second material whereby the homogeneous mixture forming any one sub-region differs from the homogeneous mixture forming immediately neighbouring sub- regions within the layer such that the index of refraction of each of the plurality of sub-regions is substantially constant with the depth of the sub-region and the index of refraction of the layer varies rapidly/sharply or substantially step-wise between successive sub-regions thereof.
  • the oscillating refractive index of the layer may be a partially, or wholly, "digitised” oscillation (e.g. a digitised wave shape) rather than a continuous oscillation ( e.g. wave) as may be the case alternatively.
  • An optical filter may form a filter for a photovoltaic cell such as a solar cell.
  • a solar cell may be formed having an optical filter comprising only an oscillating (e.g. wave) layer design (digitised or otherwise) according to the present invention in its second aspect.
  • an oscillating (e.g. wave) layer design digitalised or otherwise
  • such a wave design could be bounded by other filter layers within a stack of filter layers according to the invention in its first aspect.
  • the wave design may be applied to any one or both of the first and second inhomogeneously mixed layers of the invention in its first aspect.
  • the wave design includes a quintic shape comprising one period of a sinusoid oscillation in the refractive index of a given layer across the whole width of the layer.
  • the optical filter may be for a photovoltaic cell and such as a solar cell.
  • the present invention in its first and second aspects and accord ng to any or all of the above variants and preferable features, implements a method of producing an optical filter. Accordingly, in a third of its aspects, the present invention may provide a method of producing an optical filter, the method including: providing a substrate; stacking a plurality of layers of materials upon the substrate each of which layers is formed from one or both of: a first material having a first index of refraction; and, a second material having a second index of refraction being less than the first index of refraction; forming a first layer and a second layer of the plurality of layers from an inhomogeneous mixture of the first material and the second material; forming from the first material a third layer of the plurality of layers being stacked between said first and second layers; wherein the optical thickness of each of said first and second layers is greater than the optical thickness of said third layer.
  • the index of refraction of the first and second layer varies with the depth of the intermediate layers between values greater than the second index of refraction and less than the first index of refraction.
  • the first layer and the second layer may each be formed with an optical thickness which differs in magnitude from the value 2Q by less than Q/2 and the third layer may be formed with an optical thickness which differs in magnitude from the value Q by less than Q/2, where Q is the optical thickness of a given layer traversed by substantially of a wavelength of optical radiation of a common reference wavelength at which the optical thicknesses are determined.
  • the first layer and second layer may be formed such that the optical thicknesses thereof differ, or such that the optical thicknesses thereof are substantially equal in value. Where the first layer and the second layer are each formed to have an optical thickness of equal value, this value may be substantially equal to 2Q, or may be equal to some other value differing from 2Q by less than Q/2.
  • the third layer may be formed to have an optical thickness substantially equal to Q.
  • the method may include the step of forming a pair of outerlayers, being part of the plurality of layers, each being formed from the second material wherein the outer layers are formed with the first, second and third layers being stacked between them.
  • the pair of outer layers may be formed such that the optical thickness of each such layer differs in value from the magnitude Q by less than Q/2.
  • the optical thicknesses of each of the pair of outer layers may be substantially equal to each other, and may also be substantially equal to the value Q.
  • the method in its third aspect, may include varying the optical thickness of one, some or all of the layers in said plurality of layers for the purpose of optimising the spectral response of the optical filter for: transmitting solar radiation within a band of wavelengths to which a solar cell is operatively designed to be sensitive to, and, for reflecting solar radiation outwith said band.
  • the first and/or second layer may be formed such that the index of refraction thereof varies continuously through at least a part of the depth of the respective layer.
  • the first and/or second may be formed such that index of refraction thereof varies substantially in a step-wise manner through at least a part of the depth of the respective layer.
  • the first and/or second layer may be formed such that all variations in the index of refraction thereof occur substantially in a stop-wise manner.
  • the first and/or second layer may be formed to comprise a plurality of sub-regions each of which is formed from a homogeneous mixture of the first material and the second material whereby the homogeneous mixture forming any one sub-region differs from the homogeneous mixture forming immediately neighbouring sub-region within the first and/or second layer such that the index of refraction of each of the plurality of sub-regions is substantially constant with the depth of the sub-region and the index of refraction of the first and/or second layer varies substantially step-wise with depth between successive sub-regions thereof.
  • the first and/or second layer may be formed such that all variations in the index of refraction of the respective layer increase that index of refraction as the depth of the layer increases from regions thereof remote from the third layer to regions thereof proximate the third layer.
  • the plurality of layers are preferably arranged to form a stack of layers in which successive layers are arranged in a periodically repeating order across the depth of the stack.
  • the plurality of layers are preferably arranged to substantially reflect at least Infra-Red radiation and to transmit optical radiation at least in the visible optical spectrum.
  • the plurality of layers may be arranged to substantially reflect at least Infra-Red radiation and Ultra-violet radiation .
  • Figure 1 illustrates a transmission spectrum for a simple -viave interference-type multi-stack optical filter, the spectrum comprising a main reflection band, and a "higher order" reflection band, and reflectance ripples/oscillations in between;
  • Figures 2a, 2b and 2c illustrate the variation in refractive index of a part of a multi-layer stack of an optical filter;
  • Figure 3 illustrates a transmission spectrum for an interference-type multi-layer stack optical filter- employing multi-layer stacks of the form illustrated in Figures 2a, 2b or 2c;
  • Figure 4 illustrates a multi-layer optical filter comprising a stacked plurality of layer nests each nest being a multi-layer stack of the type illustrated in Figures 2a, 2b or 2c.
  • the spectrum illustrates the variation in the optical transmission coefficient (T) of the filter as a function of incident optical radiation wavelength ( ⁇ ) across a spectral region encompassing the operating bandwidth of a typical solar cell (e.g. from about 400 nm to about 1100 nm in optical wavelength) .
  • the transmission spectrum 1 has a main broad reflection band 2 (i.e.
  • the transmission spectrum 1 also possesses a series of optical transmission transients 4 occurring in between the main "first order" reflection band 2 and the "third order” reflection band 3, and beyond. These optical transmission transients 4 cause the transmission coefficient (T) of the optical filter to repeatedly fall significantly within the operating bandwidth of the solar cell. Both the third order reflection band 3 and the transmission transients 4 are undesirable since they exclude from use optical radiation which it is intended that the solar cell receives.
  • Figure 4 illustrates an interference-type multi-layer stack optical filter structure according to the present invention.
  • the multi-layer optical filter comprises a multi-layer stack 50 arranged upon a CMG glass substrate 60 about lOO ⁇ m thick.
  • the multi-layer stack 50 comprises a series of repeating layer groups (or "nests") each of which "nests" comprises a first and outer layer formed from a material (L) having a low refractive index (n) .
  • a succeeding second layer is formed from an inhomogeneous mixture (M) of the low-index material (L) and a different material (H) of a relatively high index of refraction.
  • the second layer has a refractive index (n) which varies with the layer's depth this being achieved by the inhomogeneity (with layer depth) of the mixture (M) of r.hfi two materials (L and H) forming the layer.
  • a succeeding third layer is formed from the high-index material (H) used in part to form the second layer.
  • a succeeding fourth layer is formed from an inhomogeneous mixture (M) of the low-index material (L) and the height index material (H) such that the refractive index of the fourth layer varies with the depth thereof as a result of inhomogeneous mixing of H and I. materials.
  • a final fifth and outer layer is formed from the same material (L) used to form the first layer.
  • each one of the second and fourth layers in the nest has an optical thickness of ⁇ --wavelength of the predetermined design wavelength. Consequently, when optical radiation of the predetermined design wavelength ( ⁇ 0 ) is propagating through any given one of the second or fourth layers within the nest, the wavelength of the radiation within that layer is substantially two times greater than the layer thickness.
  • Figure 2 illustrates the refractive index profile of any one of the multiple five-layer nests illustrated in Figure A .
  • the first and fifth layers each have the same refractive index, 20 and 24 respectively, which is low (L) and homogeneous across the depth of the respective layer.
  • the third layer has a refractive index, 22, which is high (H) and homogeneous across the depth of the layer.
  • the inhomogeneous mixture of the two materials (L and H) in question results in a refractive index (21, 23) for the second and fourth layers respectively which varies continuously with the depth of the respective layer from the lower refractive index value ( ) , through continuously changing intermediate values to the higher refractive index value (H) , the changing intermediate values being between the low value (L) associated with the first or fifth layer and the high value (H) associated with the third layer.
  • the inhomogeneous second or fourth layer thus has a ramped refractive index which increases in value from regions thereof remote from the third layer to regions thereof proximate the third layer.
  • the five-layer nest structure may be summarised as: ( MHML) .
  • optical thicknesses of successive layers illustrated in the designs of Figures 2a, 2b and 2c correspond with what may be termed a "template” or basic design arrangement which may subsequently be optimised by varying the optical thickness of one, some or all of the optical layers in one, some or all of the nests within a complete optical filter. It has been found that by varying the optical thickness of individual layers, or by varying layer optical thicknesses collectively, one may optimise the spectral response of the optical filter for the purposes of transmitting solar radiation within a band of wavelengths to which, for example, a solar cell is operative] y designed to be sensitive to, and, for optimally reflecting solar radiation outwith that band.
  • each of the second and fourth layers exceeds the opt cal thickness of the third (high-index) layer, and where present the outer (low-index) layers, by less than of the design wavelength (i.e. by less than ⁇ 0 /8) then a suitable spectral response can be achieved in the optical filte .
  • FIG. 3 there is illustrated a transmission spectrum for ⁇ multi-stack optical filter comprising seven stacked five-layer nests of the form (Q, 2Q, Q, 2Q, Q) 7 , each nest having a five-layer refractive index distribution of the form (LMHML) as illustrated in Figure 2a, 2b or 2c.
  • the region of the transmission spectrum intermediate the first order and fourth order reflection bands enjoys ⁇ high level of transmittance in which the presence of transmittance transients 32 is significantly suppressed. Furthermore, not only is the second-order reflection band completely suppressed at a wavelength of
  • the basic transmission spectrum illustrated in Figure 3 may be further improved by suitably optimising the design parameters employed in each of the seven nests of the optical filter with which the spectrum is associated. As mentioned above, this may involve suitable variations in the optical thicknesses of one, some or all of the five layers within each nest. For example, in terms of optical thicknesses, a nest may be modified to: (1.1Q, 2.3Q, 1.1Q, 2.3Q, 1.1Q). This variation is just one illustrative example of how relative thicknesses may be varied, and different variations may be applied to different nests in the multi-layer stack.
  • the gradient of the refractive index i.e. the variation of refractive index as a function of layer depth
  • the gradient of the refractive index i.e. the variation of refractive index as a function of layer depth
  • the second layer 25 and the fourth layer 26 each display a variation in refractive index which is reduced relative to that illustrated in Figure 2a.
  • each of the inhomogeneously mixed layers is formed such that the refractive index of the layer varies from a lower intermediate value (Mi) which is greater in value than the low refractive index value associated with the first layer 20, to a second intermediate value (M 2 ) greater than the first intermediate value (Mi) but less than the high-index value associated with the third layer.
  • the form of the refractive index ramp in the second and/or fourth layers need not be linear, and may be exponentially increasing (as towards the third layer) or may be some other more complex ramp shape. Indeed, a quintic ramp shape may be employed in which the refractive index of either the second or fourth layer is formed so as to gently oscillate over a single sinusoid period, the quintic oscillation being superimposed upon an underlying ramp increase in the refractive index.
  • Figure 2c illustrates a further design variant of the embodiments described herein, and shows the refractive index (n) variations of the inhomogeneously mixed second and fourth layers (27, 28) which vary substantially in a step-wise manner through the depth of the respective layer.
  • the second and fourth layer (27, 28) are each physically continuous articles, not being physically discontinuous but having a spatial distribution (inhomogeneous) of mixture (M) which causes substantially step-wise changes in the refractive index of the respective layer at certain sub-regions thereof where the mixture changes correspondingly substantially step-wise (or nearly so).
  • the second/four h layer comprises a plurality of sub-regions, such as sub-layers 65 and 70 of Figure 2c, each of which is formed from a homogeneous mixture of the first material (L) and the second material (H) over a thickness "x" of the layer.
  • the homogeneous mixture forming any one sub-region differs from the homogeneous mixture forming immediately neighbouring sub- region within the second/fourth layer (M) such that the index of refraction of each of the plurality of sub- regions is subs antially constant with the depth "x" of the sub-region.
  • the index of refraction of the second/fourth layer (M) varies substantially step-wise between successive sub-regions thereof. This amounts to a full "digitisation" of the variations in refractive index of the second and fourth layer.
  • the neighbouring sub- regions of the digitised second/fourth layers arc physically continuously formed within one physically continuous respective layer and do not represent separately formed sub-layers.
  • the inhomogeneous mixture of the two materials L & H
  • the "digitised" inhomogeneous refractive index profile illustrated in Figure 2c may be applied in place of (or in addition to) the smoothly varying index ramps of the second and fourth layers of Figures 2a and 2b. Indeed, this has been found to be easier to achieve than a smoothly varying varying refractive index ramp.
  • An advantage of such digitisation is that the formation of such digitised shapes requires less control in the apparatus used to inhomogeneously mix the two di ffaring materials employed in the mixture. The need to continuously regulate/vary the mixture is obviated when digitisation is employed.
  • Materials which may be employed in forming the layers of a multi-layer stack 50 of an optical, filter (50, 60) according to the present invention include Silicon dioxide (Si ⁇ 2 and Hafnium dioxide (HF0;>) , and a substrate glass 60 such as CMG glass.
  • the following table illustrates an example of the physical thicknesses of each of the five layers in a given five-layer nest employed in a multi-nest stack.
  • the outer first and fifth layers are each formed from Silicon dioxide, and the third high index layer is formed from Hafnium dioxide, while the second and fourth intermediate-index layers are formed from an inhomogeneous mixture of Silicon dioxide and Hafnium dioxide.
  • the refractive indices at the design wavelength are as follows :
  • each ramped layer (layers 2 and 4) of inhomogeneously mixed materials Si0 2 & Ilf0 2 is 95.7nm and in this example the refractive index of each of the two mixed layers

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  • Life Sciences & Earth Sciences (AREA)
  • Sustainable Development (AREA)
  • Engineering & Computer Science (AREA)
  • Optics & Photonics (AREA)
  • Sustainable Energy (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Electromagnetism (AREA)
  • Computer Hardware Design (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Optical Filters (AREA)
  • Laminated Bodies (AREA)

Abstract

L'invention concerne un filtre optique comprenant un substrat comportant une pluralité de couches de matériaux empilés dessus, chacun des matériaux étant formés d'une ou de deux couches: un premier matériau ayant un premier indice de réfraction, et un deuxième matériau ayant un deuxième indice de réfraction, inférieur au premier indice de réfraction, où la pluralité de couches de matériaux comprennent des première et deuxième couches chacune formée d'un mélange non homogène du premier et du second matériaux, et une troisième couche formée du premier matériau, empilée entre la première couche et la deuxième couche, où l'épaisseur optique de la première et de la deuxième couche est 2Q, et l'épaisseur optique de la troisième couche est Q, où Q est l'épaisseur de la couche indiquée traversée par un quart de longueur d'onde commune de référence, et où toutes les variations de l'indice de réfraction de la première et deuxième couches augmentent cet indice de réfraction à mesure que la profondeur de la couche respective augmente à partir des régions éloignées de la troisième couche et à partir des régions proches de la troisième couche.
PCT/EP2003/051068 2002-12-19 2003-12-18 Filtre optique WO2004061490A1 (fr)

Priority Applications (4)

Application Number Priority Date Filing Date Title
DE60312557T DE60312557T2 (de) 2002-12-19 2003-12-18 Ein optisches filter
JP2004564247A JP2006511838A (ja) 2002-12-19 2003-12-18 光学フィルタ
US10/539,623 US8018652B2 (en) 2002-12-19 2003-12-18 Optical filter
EP03809192A EP1573371B1 (fr) 2002-12-19 2003-12-18 Filtre optique

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
GB0229597A GB2396436B (en) 2002-12-19 2002-12-19 An optical filter
GB0229597.0 2002-12-19

Publications (1)

Publication Number Publication Date
WO2004061490A1 true WO2004061490A1 (fr) 2004-07-22

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PCT/EP2003/051068 WO2004061490A1 (fr) 2002-12-19 2003-12-18 Filtre optique

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Country Link
US (1) US8018652B2 (fr)
EP (1) EP1573371B1 (fr)
JP (1) JP2006511838A (fr)
DE (1) DE60312557T2 (fr)
ES (1) ES2283875T3 (fr)
GB (1) GB2396436B (fr)
WO (1) WO2004061490A1 (fr)

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JP2009520360A (ja) * 2005-12-16 2009-05-21 ザ・ボーイング・カンパニー 三重接合太陽電池のためのノッチフィルタ
US20110089338A1 (en) * 2006-05-12 2011-04-21 Semrock, Inc. Multiphoton fluorescence filters
EP2103967A4 (fr) * 2006-12-28 2012-07-04 Nippon Catalytic Chem Ind Filtre transmettant selectivement la lumiere
US8441710B2 (en) 2010-01-08 2013-05-14 Semrock, Inc. Tunable thin-film filter
US8879150B1 (en) 2009-03-20 2014-11-04 Semrock, Inc. Optical thin-film polarizing bandpass filter
US8958156B1 (en) 2007-05-30 2015-02-17 Semrock, Inc. Interference filter for non-zero angle of incidence spectroscopy
US9304237B1 (en) 2012-12-10 2016-04-05 Semrock, Inc. Tunable band-pass filter
US9323299B2 (en) 2012-08-27 2016-04-26 Green Light Industries, Inc. Multiple power source unit
US9726797B2 (en) 2012-06-04 2017-08-08 Asahi Glass Company, Limited Near-infrared cut filter

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WO2013077274A1 (fr) * 2011-11-24 2013-05-30 コニカミノルタ株式会社 Film de protection contre les infrarouges
CN104428898B (zh) * 2012-06-11 2018-05-08 赫里亚泰克有限责任公司 光活性组件的滤光系统
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CN110927853A (zh) * 2018-09-19 2020-03-27 张家港康得新光电材料有限公司 红外宽波段截止滤波器、滤光片及摄像头
CN110927850B (zh) * 2018-09-19 2022-06-03 张家港康得新光电材料有限公司 红外宽波段截止滤波器、滤光片及摄像头
EP3908863A4 (fr) 2019-03-24 2022-09-14 Spectralics Ltd. Procédé de synthèse à diffusion multiple

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US3247392A (en) * 1961-05-17 1966-04-19 Optical Coating Laboratory Inc Optical coating and assembly used as a band pass interference filter reflecting in the ultraviolet and infrared
US3423147A (en) * 1963-10-14 1969-01-21 Optical Coating Laboratory Inc Multilayer filter with wide transmittance band
US3914023A (en) * 1972-12-08 1975-10-21 Balzers Patent Beteilig Ag Wide-band multilayer interference filter
EP0567735A1 (fr) * 1992-04-30 1993-11-03 Guardian Industries Corp. Verre E du type "bas" de haute performance et durable et procédé de sa fabrication
EP0632507A2 (fr) * 1993-05-12 1995-01-04 Optical Coating Laboratory, Inc. Couverture pour cellules solaires qui réfléchit les rayons UV/IR
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Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009520360A (ja) * 2005-12-16 2009-05-21 ザ・ボーイング・カンパニー 三重接合太陽電池のためのノッチフィルタ
US20110089338A1 (en) * 2006-05-12 2011-04-21 Semrock, Inc. Multiphoton fluorescence filters
US8508849B2 (en) * 2006-05-12 2013-08-13 Semrock, Inc. Multiphoton fluorescence filters
EP2103967A4 (fr) * 2006-12-28 2012-07-04 Nippon Catalytic Chem Ind Filtre transmettant selectivement la lumiere
US8958156B1 (en) 2007-05-30 2015-02-17 Semrock, Inc. Interference filter for non-zero angle of incidence spectroscopy
US9857511B2 (en) 2007-05-30 2018-01-02 Semrock, Inc. Interference filter for non-zero angle of incidence spectroscopy
US8879150B1 (en) 2009-03-20 2014-11-04 Semrock, Inc. Optical thin-film polarizing bandpass filter
US8441710B2 (en) 2010-01-08 2013-05-14 Semrock, Inc. Tunable thin-film filter
US9726797B2 (en) 2012-06-04 2017-08-08 Asahi Glass Company, Limited Near-infrared cut filter
US9323299B2 (en) 2012-08-27 2016-04-26 Green Light Industries, Inc. Multiple power source unit
US9304237B1 (en) 2012-12-10 2016-04-05 Semrock, Inc. Tunable band-pass filter

Also Published As

Publication number Publication date
US20090025783A1 (en) 2009-01-29
EP1573371B1 (fr) 2007-03-14
US8018652B2 (en) 2011-09-13
GB2396436A (en) 2004-06-23
EP1573371A1 (fr) 2005-09-14
GB0229597D0 (en) 2003-01-22
GB2396436B (en) 2006-06-28
JP2006511838A (ja) 2006-04-06
DE60312557T2 (de) 2007-12-13
ES2283875T3 (es) 2007-11-01
DE60312557D1 (de) 2007-04-26

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